US2603418A - Electronic indicator tube - Google Patents

Description

INVENTOR 2 SHEETSSHEET 1 IO WW GATE TUBE SOURCE OF WAVE TO BE MEASURED JOSEPH C. FERGUSON J. C. FERGUSON ELECTRONIC INDICATOR TUBE FREQUENCY DlVlDER CRYSTAL CONTROLLE D WAVE SOURCE Jul 15, 1952 Filed Dec. 7, 1946 FIG. I

NEED O ATTORNEY y 15, 1952 J. c. FERGUSON v ELECTRONIC INDICATOR TUBE m E El INVENTOR JOSEPH C. FERGUSON ATTORNEY Patented July 15, 1952 UNITED STATES TENT ELECTRONIC INDICATOR TUBE Application December 7, 1946, Serial No. 714,713

3 Claims.

This invention relates generally to a frequency measuring system, and particularly pertains to an electronic tube for visually exhibiting or indicating an electrical quantity such, for example, as a voltage representative of the frequency of a wave source of unknown frequency.

A frequency measuring system has been suggested where the number of waves developed by a source of unknown frequency is counted for a predetermined time interval. To this end a plurality of impulse counter circuits are connected in cascade to count the number of waves occurring during a fixed period of time, and individual volt meters are connected to th measuring condenser of each counter circuit to measure the voltage remaining on each condenser which in turn indicates the number of waves. A measuring system of this type may also be used for measuring short time intervals by counting the number of waves of a source of known frequency during that time interval. Alternatively, irregular pulses which may be developed, for example, by a Geiger-Muller counter in response to radioactive radiation may be counted in this manner for a predetermined period of time. This measuring system has the'drawback that a separate volt meter is required for each counter circuit. The indications of the various volt meters must be converted into indications of time or frequency. It is desirable, therefore, to provide an indicator for visually and directly indicating the quantity to be measured such, for example, as a time interval or a frequency.

It has also been proposed to connect a number of decade counters in cascade, four" frequency dividers or multivibrators being required for each decade counter. Each of the multivibrators includes a neon lamp which lights whenever the multivibrator has received two impulses, the four neon lamps of the decade counted indicating, respectively,-the numerals 1, 2, 4 and 8. For each decade counter the numerals represented by the four neon lamps must be added to obtain the desired indication. This measuring circuit is therefore complicated in view of the large number of component circuit elements required and the desired indication such, for example, as the frequency of a wave can only be derived by computation.

It is an object of the present invention, therefore, to provide a novel electronic indicator tube for visually indicating an electrical quantity such, for example, as a voltage.

Another object of the invention is to provide 2 a novel tube of the cathode ray type for visually exhibiting the frequency of a wave source of unknown frequency measured by counting thenumber of waves occurring during a predetermined length of time, or for indicating short time intervals which are measured by counting the number of waves of a source of known frequency during the time interval to be measured.

A further object of the invention is to provide an electronic indicator for selectively exhibiting letters, numerals or symbols indicating, for example, a voltage which may be representatlilve of the frequency of a wave source or the 1' e.

In accordance with the present invention there is provided an electronic indicator comprising a cathode including means for developing a plurality of electron beams. Each of the beams has a cross section representing a character such as a symbol, a letter, or a numeral. There are further provided a luminescent screen and means for focusing the electron beams on the screen. Finally, means are provided for selecting one of the electron beams and for directing it toward the luminescent screen in accordance with an electrical quantity to be indicated which may, for example, be a. voltage.

For a better understanding of the invention, together with other and further objects thereof, reference is made to the following description, taken in connection with the accompanying drawings, and its scope will be pointed out in the appended claims.

In the accompanying drawings:

Fig. 1 is a schematic circuit diagram, partly in block form, of a frequency measuring system in accordance with the invention including an electronic indicator tube sectioned on line l-| of Fig. 3;

Fig. 2 is a graph showing the voltage wave developed across the measuring condenser of one of the counter circuits forming part of the frequency measuring system of Fig. 1;

Fig. 3 illustrates an electronic indicator tube embodying the present invention;

Fig. 4 is a view on enlarged scale taken on line 4-4 of Fig. 3 and illustrating the cathode of the indicator tube;

Fig. 5 is a view taken on line 5-5 of Fig. 3 of Cthe luminescent screen of the indicator tube; an

Fig. 6 illustrates another embodiment of the indicator tube of the invention.

Referring to the drawings, in which like comsignee of the instant application.

3 ponents are designated by the same reference numerals throughout the figures, and particularly to Fig. 1, there is illustrated a frequency measuring system comprising source I of a Wave, the frequency of which is to be measured. In order to measure the frequency of the wave developed by source 1 the number of waves developed by the source is counted for a predetermined interval of time. For the purpose of establishing the predetermined time interval there is provided wave source 2 of which is preferably crystal controlled and the frequency of Whichis known. The frequency of the wave developed by standard frequency source 2 is divided by fre.--

euency divider 3 which operatesto develop an output pulse indicated at 4 which has a. predetermined duration such, for examplaas one second.

The wave of unknown frequency developed by source l is impressed upon a normally inoperative gate tube schematically indicated at 5. Gate tube 5 is rendered operative by applying thereto pulse 4 developed by frequency divider 3. Gate tube 5 accordingly passes the wave developed by source I for a predetermined time interval which and claimed in copending application Serial No.

665,659, filedon April 29, 1946, now Patent No. 2,583,003, in the name of L. F. Mayle, entitled Counter Circuit and assigned to the assignee of the present application. It is, however, to be understood that any conventional impulse'counter circuit may be substituted for impulse counters s and l illustrated in Fig. 1. Preferred im pulse'counters which may be substituted for those illustrated in Fig. 1 have been disclosed and claimed in copendin'g'v applications, Serial No. 665,594, now abandoned, to L. F. Mayle entitled Impulse Counter Circuit and Serial 'No. 665,593 to C. E. Hallmark entitled Pulse Counter, both filed on April 27, 1946 and assigned to the as- 25. Anode 25 is connected through winding 26 of transformer 21 to anode voltage supply 3+. The other winding 28 of transformer 2'! is connected between cathode impedance [8 and measuring condenser l2, on the one hand, and con trol grid 24 of blocking oscillator 22, on the other hand. Cathode resistor 39 of blocking oscillator 22 is provided between cathode 2 3 and ground as illustrated; The output signal at areduced frequency may be obtained from output lead 3% connected between cathode 23 and cathode resisorder of 10 volts or more.

Impulse counter 8 includes charging condenser H 'and' measuring condenser l2 connected in increments in response to input waves 19, there is provided space discharge tube l4 comprising cathode 15, control grid 13 and anode I! which may be connected to a suitable anode voltage source indicated at 13+. For the purpose of providing self-bias, impedance 18 may be provided between cathode l5 and measuring condenser i2.

Cathode impedance l8 comprises adjustable resistor 20 and condenser 2! arranged in parallel. Discharge tube I4 is accordingly normally biased to cutoff.

For the purpose of periodically bringing measuring condenser I2 we predetermined negative potential there is provided blockingoscillator 22 comprising cathode 23, control grid 24 and anode tor 38. Output lead 3! may be connected to charging condenser 33 of impulse counter l which is identical to impulse counter 6.

Input waves'or' pulses It should be of positive polarity and should have an amplitude of the The output signal obtained from output lead 3| is also of positive polarity. Impulse counter 6 operates as follows.

Let it be assumed that initially measuring condenser !2 is driven by blocking oscillator 22 to a high negative potential which may be'of the order of 500 volts. To this, end the terminal of measuring condenser 12 connected to cathode impedance [8 may be momentarily connected to ground by a switch 35, thereby to discharge condenser [2. This Will fire blocking oscillator 22 in a manner to be'explained hereinafterand will impress a negative potentialupon measuring condenser 12. Since chargingcondenser II and measuring condenser [2 are connected through resistor 13, the voltage on condensers II and 12 will equalize so that both condensers will acquire a high negative-voltage. Controlgrid 24 of blocking oscillator 22 is held at this negative voltage by measuring condenser 12,. thereby biasing blocking oscillator 22 .considerably beyond cutoif. In view of the self-bias voltage developed across cathode impedance l8 dischargetube It is also cutoff.

Upon the arrival of'the leading'edge or" the first wave of wave-train luwhich is of positive polarity, the voltage of charging condenser H is raised toward ground, thereby driving control grid lB-positive with respect to cathode l5. Discharge tube lt will accordingly begin to conduct space current and will charge measuring condenser -l2. While tube conducts space current, the voltage of measuring condenser [22 is raised toward ground until discharge tube l4 ceases again to conduct space current. Tube M is out 01f again as soon as the voltage of measuring condenser [2, that is, of cathode I5 is raised by a sufficient voltage increment which preferably The conduction of discharge tube M is controlledby the voltages across l4, while-the major portion of the energy sup- "plied to measuring condenserlZ isfurnished i by the space current fiowing'through tube l4.

' Upon the arrival of the'trailing edge of the first input wave, the voltage across charging condenser it is depressedagain to a more negative value thanv its initial voltage, thus driving controlgrid It considerably beyond cutoff. --At this time the voltage at the junction point of charging condenser H and resistor i3 is negative with respect to that at thev junction point between-resistor I3 and measuring condenser l2.

age drop across measuring condenser l2, occurring between the arrival of successive input waves, the capacitance of measuring condenser |2 should preferably be large compared to that of charging condenser H.

In response to successive input Waves the'voltage across measuring condenser l2 will increase Joy substantially equal voltage increments, as illustrated by curve 31 of Fig. 2. After a predetermined number of input Waves has been impressed upon charging condenser H, the voltage across measuring condenser l2 has been raised sufiiciently to fire blocking oscillator 22 in view of the fact that measuring condenser I2 is coupled between control grid 24 and cathode 23 of the blocking oscillator. During a cycle of oscillation of blocking oscillator 22, a negative voltage is developed across winding 28 of transformer 21 which is impressed upon measuring condenser l2 and subsequently through resistor |3 upon charging condenser At the same time an output signal is developed across cathode resistor 30 of blocking oscillator 22 which is impressed through output lead 3| upon charging condenser 33 of impulse counter 1.

Although count-down ratios of 70 to 1 have been obtained with an impulse counter such as shown at 6, the counter circuits are preferably arranged to have a count-down ratio of to 1 only so that impulse counters 6 and 1 function as decade counters. The count-down ratio of the impulse counters such as counter 6 is determined principally by the negative voltage impressed at the end of each counting cycle by blocking oscillator 22 upon measuring condenser l2 and upon the voltage increments developed across measuring condenser [2 in response to each input wave. These voltage increments depend in turn upon the voltage of input Wave train II] which accordingly should be of the order of 10 volts or more.

Impulse counter 1 is identical with counter 6 so that no further explanation of its operation is required. An output signal may be obtained from output lead 40 of impulse counter 1 which may, if desired, be applied to the charging condenser of another decade counter identical to impulse counters 6 and 1.

Let it be assumed that impulse counters 6 and 1 are arranged as decade counters. In that case the voltage remaining on the measuring condensers of the impulse counters indicates the number of Waves to be counted. Thus, the voltage remaining on measuring condenser I2 of impulse counter 6, which is the first decade counter, indicates the units of the number of waves, while the voltage remaining on measuring condenser 4| of impulse counter 1, which is the second decade counter, indicates the number of waves in units of 10. The voltage remaining on the measuring condenser of a third decade counter would indicate the number of waves in units of 100, etc. Accordingly, in order to obtain an indication of the number of waves contained in wave train l0 all that needs to be done is to measure the voltages remaining on the measuring condensers of the decade counters such as l2 and 4|.

For the purpose of exhibiting visually these voltages which, in turn, indicate the number of waves contained in wave train In there is provided in accordance with the present invention electronic indicator 45 illustrated in greater detail in Fig. 3. Indicator 45 illustrated in Fig. 1 is a view taken on line of Fig. 3. Electronic indicator 45 is provided with cathode 46 which may be connected to th negative terminal of a suitable voltage source, such as battery 41 having its positive terminal grounded, as shown. As illustrated in Fig. 4, cathode 46 may bear photosensitive areas 50, each of which represents a character such as a symbol, a letter or a numeral. As shown in Fig. 4, the photosensitive areas 50 are arranged in a number of adjacent rows 5|, 52 and 53, each row representing the numerals from zero to nine, inclusive. It is to be understood that any number of rows of photosensitive areas may be provided, three rows being shown by way of example only.

Photosensitive areas 50 on cathode 46 are energized by light source 55, the light of which may be focused on cathode 46 by lens system 56. Photosensitive areas 50 may be provided on cathode 46 in any suitable manner such, for example, as by embossing. It is also feasible to provide cathode 46 with a continuous photosensitive surface. In that case the desired characters or numerals may be projected by means of light source 55 and lens system 56 on cathode 46 through film 51 which may have transparent areas arranged in rows, each area representing a desired character.

In this manner a plurality of electron beams are developed on electronic indicator 45, each of the beams having a cross section representing a character such as a numeral. The electron beams are focused on luminescent screen 58 by means of focusing coil 66 which may be energized from a suitable current source such as battery 6|. Luminescent screen 58 may be grounded as illustrated.

Luminescent screen 58 preferably has a height, as shown in Figs. 3 and 5, which is sufiicient to exhibit only one of the numerals represented by areas 5|].

In accordance with the present invention the electron beams developed from photosensitive areas 56 are deflected across luminescent screen 58. To this end there are provided deflecting elements or plates 63, 64 and 65 (Fig. 1), each being associated with one row 5|, 52 and 53, respectively, of photosensitive areas 50. The second defiecting plate 66 may be common to deflecting elements 63, 64 and 65 and may be grounded as illustrated.

As shown in Fig. l, deflecting plate 63 of indicator tube 45 is connected to measuring condenser l2 of impulse counter 6 by lead 61. Deflecting plate 63 is associated with row 5| of the photosensitive areas 50. Similarly, deflecting plate 64 associated with row 52 is connected to measuring condenser 4| of impulse counter 1 through lead 68. Lead 69 connected to deflecting plate 65 associated with row 53 may be connected to the measuring condenser of the next decade counter which may be connected to impulse counter 1.

The operation of electronic indicator 45 will now be evident. The voltages remaining on measuring condensers l2 and 4| of impulse counters 6 and 1, respectively, indicate the number of waves of wave train l0. Let it be assumed that wave train l0 includes 275 waves. Impulse counter 6 will accordingly count 2'75 waves. Every time ten waves have been impressed on counter 6, blocking oscillator 22 will fire so that the oscillator is triggered twenty-seven times. The last five waves impressed on counter 6 will build up a voltage across measuring condenser l2 which therefore corresponds to five steps of staircase wave 31 of Fig. 2. This voltage which remains on condenser l2,,is now impressed on deflecting element 53 to deflect the electron beams corresponding to row across luminescent screen 58 until numeral 5 is focused on this screen.

Impulse counter 1 receives twenty-seven input waves or pulses, and accordingly, measuring condenser il has a voltage remaining thereon corresponding to seven steps of staircasewave 31. This voltage is impressed on deflecting element 64 to deflect the second row of electron beams corresponding to row 52 across luminescent screen 58 so that numeral 1 will be visible on screen 58. The blocking oscillator of impulse counter 1 is fired twice so that two impulses would be received by an impulse counter connected to counter 7. The voltage remaining on the measuring condenser of a third counter may be impressed through lead 69 on deflecting element 65 to deflect the third row of electron beams corresponding to row 5 3 across luminescent screen 58 to exhibit the numeral 2, as illustrated in Fig. 5. The numerals 2, 7, 5 appearing on screen 53 and indicating 2'75 waves of source 1 are therefore exhibited in a horizontal line which greatly facilitates the rapid observation of the result of the measurement.

As pointed out hereinbefore, impulse counters 5 and 7 develop a staircase wave of negative polarity across their respective measuring condensers l2 and 4!. Electronic indicator will also operate in connection with a counter circuit wherein a staircase wave of positive polarity is developed. Such an impulse counter has been disclosed, for example, in copending application Serial No. 665,591 to L. F. Mayle referred to hereinabove.

The electronic indicator of the present invention may be utilized for measuring the frequency of a wave of unknown frequency in the manner explained in connection with Fig. 1. .Thus, wave source I may be an audio source or it may be a frequency standard, the frequency of which is to be checked. The frequency measuring system of Fig. 1 may also be used with advantage for the alignment of receivers, that is, for providing proper tracking between the tuning elements of the receiver and the frequency indication on the dial.

The system of Fig. 1 may furthermore be used for measuring short time intervals. For that purpose gate tube 5 may be directly connected to standard frequency source 2, the frequency of which is known. By opening gate tube 5 during the time interval, the length of which is to be measured, the number of waves developed by standard frequency source 2 may be counted during the unknown time interval. This in turn will give a direct indication of time. One of the main advantages of electronic indicator 45 is that the quantity to be measured is directly indicated on luminescent screen 58 and that all. the numerals a pear on screen 58 in a horizontal line. It is not necessary to carry out any computations, and the indicator tube may be connected to any number of counter circuits.

The electronic indicator of the present invention may also be connected to an electronic computing device for visually indicating the quantity to be measured. Indicator tube 55 may furthermore be utilized for exhibiting letters in the manner of a teletypewriter. In that case cathode 45 of tube should be provided with one row of photosensitive areas, each area representing a letter of the alphabet. If the input wave impressed upon one of the deflecting elements of the tube has a voltage which is representative of one of the letters in the alphabet, the desired letter will be exhibited on luminescent screen 58 by electrostatic deflection.

Referring now to Fig. 6, there is illustrated a modification of this invention comprising electronic indicator 19 including cathode H. Cathode ll consists of a heat conducting material such as a metallic sheet which is not thermionic emissive. Cathode H may be provided in any suitable manner with a number of' thermionic emissive areas having predetermined configurations similar to photosensitive areas 56 of cathode 46 (Fig. 4). The thermionic emissive areas provided on cathode 7| may be energized by heater (2 which heats cathode H and its thermionic emissive areas and is connected across a suitable current source such as battery 13. The thus developed electron beams may be focused on luminescent screen M by focusing coil 60 and may be deflected by deflecting plates 15 in the manner previously explained. Luminescent screen '14 may extend across the entire height of the tube, the undesired electrons being collected by anode l6 having an aperture or slot ll through which the desired electron beams may pass. Electronic indicator operates in the same manner as indicator 45.

While there has been described what is at present considered the preferred embodiment of the invention, it will be obvious to those skilled in the art that various changes and modifications may be made therein without departing from the invention, and it is, therefore, aimed in the appended claims to cover all such changes and modifications as fall within the true spirit and scope of the invention.

What is claimed is:

1. An electronic indicator tube comprising a cathode, said cathode including means for developing a plurality of electron beams arranged in adjacent rows each of said beams having a cross section representing a character, a luminescent screen, means for focusing said beam on said screen, a plurality of electrostatic deflecting plates equal in number to the number of rows,

- each of said plates being mounted in alignment with a separate one of said rows and adapted upon application of a voltage thereto to deflect the beams in its associated row so that a selected one of the beams in this row falls upon the luminescent screen. i

2. An electronic indicator tube according to claim 1 wherein the means for developing a plurality of electron beams comprises an equal number of photosensitive areas formed on cathode at, each of said areas representing a character.

3. In a frequency counting and indicating system, the combination of a plurality of counters connected in cascade for counting the frequency of a given electrical phenomena, each of said counters including a measuring condenser across which a voltage is developed representing the digital value of the denominational order measuredby said counter, a frequency indicating tube comprising a plurality of electron beam emitters arranged in rows, each row corresponding to a given denominational order and each emitter in a given row representing a different digit, a plurality of separate deflecting electrodes each ailgne d with a separate one of said rows and adapted to deflect the beams of said row, a luminescent member towards which all of said beams are directed, and means for applying the voltage from each of said condensers to a separate corresponding one of said deflecting electrodes to deflect the beams-in each row according to the potential oi the condenser so that a selected beam Number in each row strikes the luminescent material. 2,283,383 JOSEPH C. FERGUSON. 2,310,105 2,354,768 REFERENCES CITED 5 2,405,597 The following references are of record in the 2, ,698 file of this patent: 2,436,963 UNITED STATES PATENTS 2455639 Number Name 10 1,072,426 Claflin Sept. 9, 1913 Number 2,267,827 Hubbard Dec. 30. 1941 355.705

Name Date McNaney May 19, 1942 Michel "Feb. 2, 1943 Nokes Aug. 1, 1944 Miller Aug. 13, 1946 Miner -l: June 24, 1947 Crosdofi Mar. 2, 1948 Anderson Dec. 7, 1948 FOREIGN PATENTS Country Date Great Britain Aug. 24, 1931

Images